Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 4244 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{2}M_{8}$ | 0.6658 | 0.8419 | 0.7909 | [M:[1.1831, 0.7605, 0.8169, 0.8169, 0.8169, 0.7887, 0.7323, 1.2395], q:[0.8028, 0.4367], qb:[0.3803, 0.8028], phi:[0.3944]] | [M:[[-6], [-14], [6], [6], [6], [-4], [-24], [14]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{7}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{8}$, ${ }q_{1}q_{2}$, ${ }M_{7}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{7}M_{8}$, ${ }M_{7}q_{1}q_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ | ${}\phi_{1}\tilde{q}_{2}^{2}$ | -3 | t^2.197 + 2*t^2.366 + 3*t^2.451 + t^3.465 + 2*t^3.718 + t^4.394 + 2*t^4.563 + 3*t^4.648 + 3*t^4.732 + 7*t^4.817 + 6*t^4.901 + t^5.662 + t^5.831 + 3*t^5.915 - 3*t^6. + 2*t^6.085 + 5*t^6.169 + t^6.591 + 2*t^6.76 + 3*t^6.845 + 4*t^6.929 + 6*t^7.014 + 7*t^7.099 + 9*t^7.183 + 10*t^7.268 + 7*t^7.352 + 2*t^7.437 + t^7.859 + t^8.028 + 3*t^8.112 - 2*t^8.197 + t^8.282 - 2*t^8.366 - 9*t^8.451 + 4*t^8.535 + 8*t^8.62 + t^8.788 + 2*t^8.957 - t^4.183/y - t^6.38/y - (2*t^6.549)/y - (2*t^6.634)/y + (2*t^7.563)/y + (3*t^7.648)/y + (3*t^7.732)/y + (8*t^7.817)/y + (3*t^7.901)/y + t^7.986/y - t^8.577/y + t^8.662/y - (2*t^8.746)/y + (2*t^8.915)/y - t^4.183*y - t^6.38*y - 2*t^6.549*y - 2*t^6.634*y + 2*t^7.563*y + 3*t^7.648*y + 3*t^7.732*y + 8*t^7.817*y + 3*t^7.901*y + t^7.986*y - t^8.577*y + t^8.662*y - 2*t^8.746*y + 2*t^8.915*y | t^2.197/g1^24 + (2*t^2.366)/g1^4 + 3*g1^6*t^2.451 + t^3.465/g1^16 + 2*g1^14*t^3.718 + t^4.394/g1^48 + (2*t^4.563)/g1^28 + (3*t^4.648)/g1^18 + (3*t^4.732)/g1^8 + 7*g1^2*t^4.817 + 6*g1^12*t^4.901 + t^5.662/g1^40 + t^5.831/g1^20 + (3*t^5.915)/g1^10 - 3*t^6. + 2*g1^10*t^6.085 + 5*g1^20*t^6.169 + t^6.591/g1^72 + (2*t^6.76)/g1^52 + (3*t^6.845)/g1^42 + (4*t^6.929)/g1^32 + (6*t^7.014)/g1^22 + (7*t^7.099)/g1^12 + (9*t^7.183)/g1^2 + 10*g1^8*t^7.268 + 7*g1^18*t^7.352 + 2*g1^28*t^7.437 + t^7.859/g1^64 + t^8.028/g1^44 + (3*t^8.112)/g1^34 - (2*t^8.197)/g1^24 + t^8.282/g1^14 - (2*t^8.366)/g1^4 - 9*g1^6*t^8.451 + 4*g1^16*t^8.535 + 8*g1^26*t^8.62 + t^8.788/g1^96 + (2*t^8.957)/g1^76 - t^4.183/(g1^2*y) - t^6.38/(g1^26*y) - (2*t^6.549)/(g1^6*y) - (2*g1^4*t^6.634)/y + (2*t^7.563)/(g1^28*y) + (3*t^7.648)/(g1^18*y) + (3*t^7.732)/(g1^8*y) + (8*g1^2*t^7.817)/y + (3*g1^12*t^7.901)/y + (g1^22*t^7.986)/y - t^8.577/(g1^50*y) + t^8.662/(g1^40*y) - (2*t^8.746)/(g1^30*y) + (2*t^8.915)/(g1^10*y) - (t^4.183*y)/g1^2 - (t^6.38*y)/g1^26 - (2*t^6.549*y)/g1^6 - 2*g1^4*t^6.634*y + (2*t^7.563*y)/g1^28 + (3*t^7.648*y)/g1^18 + (3*t^7.732*y)/g1^8 + 8*g1^2*t^7.817*y + 3*g1^12*t^7.901*y + g1^22*t^7.986*y - (t^8.577*y)/g1^50 + (t^8.662*y)/g1^40 - (2*t^8.746*y)/g1^30 + (2*t^8.915*y)/g1^10 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 2245 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ | 0.6847 | 0.8767 | 0.781 | [M:[1.1784, 0.7496, 0.8216, 0.8216, 0.8216, 0.7856, 0.7136], q:[0.8036, 0.4468], qb:[0.3748, 0.8036], phi:[0.3928]] | t^2.141 + t^2.249 + 2*t^2.357 + 3*t^2.465 + t^3.427 + t^3.751 + t^4.282 + t^4.39 + 3*t^4.498 + 5*t^4.606 + 6*t^4.714 + 7*t^4.822 + 6*t^4.93 + t^5.568 + t^5.676 + t^5.784 + 2*t^5.892 - 2*t^6. - t^4.178/y - t^4.178*y | detail |